You've presumable seen that \zeta(s)=\sum_{n=1}^{\infty}n^{-s}, valid when the real part of s is greater than 1. If you try to put in something with real part less than 1, this series diverges, I'm sure you've seen the harmonic series, this is just \zeta(1).
Using some analytical trickery (which you may or may not find simple or intuitive), it turns out it's possible to find a function f(s) that is valid for any complex number s (except a "pole" at s=1) and has the property that f(s)=\zeta(s) whenever the real part of s is greater than 1. Since this function f agrees with Zeta where Zeta is defined by it's Dirichlet series (that infinite sum above), we're going to use this f to define Zeta for all complex values. This what's meant by analytic continuation, and it turns out there's only one analytic continuation of Zeta to the entire complex plane.
So, using this f(s) it's possible to any value of Zeta we like, such as \zeta(0)\equiv f(0)=-1/2, \zeta(-1)\equiv f(-1)=-1/12, \zeta(-2)\equiv f(-2)=0 (I'm using \equiv to mean "defined as"). If you were to blindly substitute these s values into the Dirichlet series and ignore matters of convergence, you get the equations you've written.
Don't read much into this. For a simple analogy, consider the function g(x)=x/x. This is undefined at x=0 and the constant 1 everywhere else. Set f(x)=1. In a similar sense to our analytic continutation of Zeta above, f(x) is a continuation of g(x) to the entire real line, so we can now define some reasonable value of g at x=0, namely g(0)\equiv f(0)=1. Same as above, if we ignore the initial defects our formula for g(x) had at 1, we get the equation 0/0=g(0)=1. This is a bit of nonsense of course, if you've taken any calculus you should know the dangers of 0/0.